Light-emitting system

ABSTRACT

A standard direction (S) is a horizontal direction (a direction along X direction in the drawing). A base material ( 200 ) is supported by a frame body ( 250 ) so that a second surface ( 204 ) of the base material ( 200 ) is oriented obliquely upward from the standard direction (S). Thereby, a reference direction (R) is oriented obliquely upward from the standard direction (S). Light from the light-emitting system ( 20 ) has standard chromaticity in the standard direction (S). In addition, the light from the light-emitting system ( 20 ) has first chromaticity and second chromaticity in a first side direction (S 1 ) and a second side direction (S 2 ), respectively, the first side direction (S 1 ) and the second side direction (S 2 ) being symmetric with respect to the standard direction (S). A difference between the first chromaticity and the standard chromaticity is smaller than a difference between the second chromaticity and the standard chromaticity.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a U.S. National Stage entry of PCT Application No: PCT/JP2016/070609 filed Jul. 12, 2016, the contents of which are incorporated herein by reference.

TECHNICAL FIELD

The present invention relates to a light-emitting system.

BACKGROUND ART

In recent years, organic light-emitting diodes (OLEDs) having a microcavity structure have been developed. Such OLEDs include a reflecting layer, a semi-transparent reflecting layer, and an organic layer. The organic layer is between the reflecting layer and the semi-transparent reflecting layer and emits light. The light from the organic layer is reflected between the reflecting layer and the semi-transparent reflecting layer and emitted from the semi-transparent reflecting layer side.

Patent Document 1 describes an example of OLEDs having a microcavity structure. The OLED described in Patent Document 1 is formed so that a distance L between the reflecting layer and the semi-transparent reflecting layer satisfies 2L/λ+φ/(2π)=m (m is an integer) (A: a wavelength of light from the organic layer, φ: a phase shift amount generated in the reflecting layer and the semi-transparent reflecting layer, m: an integer).

Patent Document 2 describes an example of OLEDs having a microcavity structure. The OLED described in Patent Document 2 includes a scattering member which scatters light emitted by the microcavity structure. In Patent Document 2, the light scattered by the scattering member is emitted from the OLED.

Patent Document 3 describes an example of OLEDs having a microcavity structure. The OLED described in Patent Document 3 includes a substrate having a concave portion. The microcavity structure is formed in the concave portion of the substrate. Patent Document 3 describes that an emitting range of light emitted from the OLED becomes wider due to the concave portion.

RELATED ART DOCUMENT Patent Documents

[Patent Document 1]: Japanese Unexamined Patent Application Publication No. 2006-147598 [Patent Document 2]: Japanese Unexamined Patent Application

Publication No. 2000-284726 [Patent Document 3]: Japanese Unexamined Patent Application Publication No. H09-190883

SUMMARY OF THE INVENTION

The OLED having a microcavity may be inclined from a specific standard direction (for example, the horizontal direction.) In such a case, a reduction may be required in a difference between chromaticity on one side of the standard direction and chromaticity in the standard direction.

An example of the problem to be solved by the present invention is to reduce a difference between chromaticity on one side of a standard direction and chromaticity in the standard direction even when an OLED having a microcavity is inclined from the standard direction.

Means for Solving the Problem

The invention described in claim 1 is a light-emitting system including:

a light-emitting unit having a resonator and an organic layer interposed in the resonator, the light-emitting unit inclined from a standard direction,

in which a light distribution of light from the light-emitting unit has a higher luminous intensity in the standard direction compared to that in a reference direction along a width direction of any of the light-emitting unit, the resonator, or the organic layer,

in which the light from the light-emitting unit comprises standard chromaticity in the standard direction, and first chromaticity and second chromaticity in a first side direction and a second side direction, respectively, the first side direction and

the second side direction being symmetric with respect to the standard direction, and

in which a difference between the first chromaticity and the reference chromaticity is smaller than a difference between the second chromaticity and the reference chromaticity.

BRIEF DESCRIPTION OF THE DRAWINGS

The objects described above, and other objects, features and advantages are further made apparent by suitable embodiments that will be described below and the following accompanying diagrams.

FIG. 1 is a diagram of a light-emitting device according to an embodiment.

FIG. 2 is a diagram to explain a movement of the light-emitting device illustrated in FIG. 1.

FIG. 3 is a diagram to explain the derivation of Formula (1).

FIG. 4 is a flowchart to explain an example of a method of designing the light-emitting device illustrated in FIG. 1 and FIG. 2.

FIG. 5 is a table showing an example of the light-emitting device illustrated in FIG. 1 and FIG. 2.

FIG. 6 is a table showing a refractive angle in each layer of the light-emitting device illustrated in FIG. 5.

FIG. 7 is a table to explain an example of a method of designing the light-emitting device shown in FIG. 5 using the method shown in FIG. 4.

FIG. 8 is a graph showing a light distribution of the light-emitting device designed under the conditions shown in FIG. 7 using rectangular coordinates.

FIG. 9(a) is a graph showing an angular distribution of chromaticity (x) of the light-emitting device designed under the conditions shown in FIG. 7, and

FIG. 9(b) is a graph showing an angular distribution of chromaticity (y) of the light-emitting device designed under the conditions shown in FIG. 7.

FIG. 10 is a graph showing a spectral distribution of each of a light-emitting device according to an embodiment and a light-emitting device according to a comparative example.

FIG. 11(a) is a graph (a distribution curve) showing a light distribution of each of a light-emitting device according to an embodiment and a light-emitting device according to a comparative example using polar coordinates, and

FIG. 11(b) is a graph showing each light distribution shown in FIG. 11(a) using rectangular coordinates.

FIG. 12(a) is a graph showing an angular distribution of chromaticity (x) of each of a light-emitting device according to an embodiment and a light-emitting device according to a comparative example, and

FIG. 12(b) is a graph of an angular distribution of chromaticity (y) of each of a light-emitting device according to an embodiment and a light-emitting device according to a comparative example.

FIG. 13(a) is a graph (a distribution curve) of a light distribution of a light-emitting device according to a modification example using polar coordinates, and

FIG. 13(b) is a graph showing a light distribution shown in FIG. 13(a) using rectangular coordinates.

FIG. 14 is a diagram showing a first modification example of FIG. 1.

FIG. 15 is a diagram showing a second modification example of FIG. 1.

FIG. 16 is a diagram showing a third modification example of FIG. 1.

FIG. 17(a) is a diagram to explain a first example of a reference direction shown in FIG. 2,

FIG. 17(b) is a diagram to explain a second example of the reference direction shown in FIG. 2, and

FIG. 17(c) is a diagram to explain a third example of the reference direction shown in FIG. 2.

FIG. 18 is a plan view of a light-emitting device according to Example 1.

FIG. 19 is a cross-sectional view taken along line A-A of FIG. 18.

FIG. 20 is a cross-sectional view taken along line B-B of FIG. 18.

FIG. 21 is a diagram of a first modification example of FIG. 19.

FIG. 22 is a diagram of a second modification example of FIG. 19.

FIG. 23 is a diagram of a light-emitting system according to Example 2.

FIG. 24 is a cross-sectional view taken along line A-A of FIG. 23.

FIG. 25 is a cross-sectional view taken along line B-B of FIG. 23.

FIG. 26 is a diagram to explain an example of a light distribution of the light-emitting system shown in FIG. 25.

FIG. 27(a) is a diagram to explain an example of an angular distribution of chromaticity (x) of a light-emitting system shown in FIG. 25, and

FIG. 27(b) is a diagram to explain an example of an angular distribution of chromaticity (y) of a light-emitting system shown in FIG. 25.

FIG. 28 is a diagram to explain a first example of a method of measuring a light distribution of light from a light-emitting region (a light-emitting unit).

FIG. 29 is a diagram to explain a second example of a method of measuring a light distribution of light from a light-emitting region (a light-emitting unit).

FIG. 30 is a diagram of a modification example of FIG. 25.

FIG. 31 is a diagram of a first modification example of FIG. 24.

FIG. 32 is a diagram of a second modification example of FIG. 24.

FIG. 33 is a diagram of a third modification example of FIG. 24.

FIG. 34 is a cross-sectional view of a light-emitting system according to Example 3.

FIG. 35 is a diagram of a modification example of FIG. 34.

FIG. 36 is a cross-sectional view of a light-emitting system according to Example 4.

FIG. 37 is a cross-sectional view of a light-emitting system according to Example 4.

FIG. 38 is a diagram of a mobile object according to Example 5.

DESCRIPTION OF EMBODIMENT

An embodiment of the present invention will be described below by referring to the drawings. Moreover, in all the drawings, the same constituent elements are given the same reference numerals, and descriptions thereof will not be repeated. Further, in a range of the present specification, drawings, and patent claims, “above”, “below”, or “between” is a description regarding a positional relationship, and whether directly being in contact or not is not limited unless otherwise indicated.

FIG. 1 is a diagram showing a light-emitting device 10 according to the embodiment. FIG. 2 is a drawing explaining the operation of the light-emitting device 10 shown in FIG. 1. The light-emitting device 10 includes a reflecting layer 152, a semi-transparent reflecting layer 154, and an organic layer 120. The organic layer 120 is between the reflecting layer 152 and the semi-transparent reflecting layer 154. The organic layer 120 includes a light-emitting layer (EML) 126. A light distribution of light from the light-emitting device 10 has a higher luminous intensity in a first direction D1 that is different from a reference direction R compared to the luminous intensity in the reference direction R. The reference direction R is a central direction of the light distribution of the light-emitting device 10 (or a later described light-transmitting region 242 or a light-emitting unit 172), and in an example shown in FIG. 2, for example, is a direction along the thickness direction of a substrate 100, a direction along the thickness direction of each layer (for example, the EML 126) of a resonator 150, or a normal direction of a second surface 104 of the substrate 100. In addition, the light distribution has a higher luminous intensity also in a second direction D2 which is on an opposite side of the first direction D1 with respect to the reference direction R compared to the luminous intensity in the reference direction R. In the example shown in FIG. 2, the first direction D1 and the second direction D2 are symmetric with respect to the reference direction R. Particularly in the example shown in FIG. 2, the light distribution has a maximum value in each of the first direction D1 and the second direction D2.

More specifically, the light-emitting device 10 includes k layers of layers 156 (k is an integer which is equal to or greater than 2) which are from a first layer 156 (1) to the k-th layer 156 (k). In the examples shown in FIG. 1 and FIG. 2, k is 5. These layers 156 are between the reflecting layer 152 and the semi-transparent reflecting layer 154. In the light-emitting device 10, a value ΔM which is defined by Formula (1) below is equal to or greater than m−⅛ and equal to or less than m+⅛ (m is an integer which is equal to or greater than 1). A detailed description will be provided below.

$\begin{matrix} {\left\lbrack {{Formula}\mspace{20mu} 1} \right\rbrack\mspace{619mu}} & \; \\ {{\Delta\; M} = {{\frac{2}{\lambda}{\sum\limits_{i = 1}^{k}{d_{i}\sqrt{n_{i}^{2} - {n_{0}^{2}\sin^{2}\theta_{0}}}}}} + {\frac{1}{2\pi}\left( {\phi_{S} + \phi_{R}} \right)}}} & (1) \end{matrix}$ λ: Peak wavelength of light from EML 126 d_(i): Thickness of i-th layer 156 (1≤i≤k) n_(i): Refractive index of i-th layer 156 (1≤i≤k) n₀: Refractive index of medium propagated by light from light-emitting device 10 (or second surface 102 of substrate 100) θ₀: Angle of direction at which above-mentioned light distribution has maximum value φ_(S): Phase shift amount of semi-transparent reflecting layer 154 φ_(R): Phase shift amount of reflecting layer 152.

The light-emitting device 10 includes a substrate 100, a first electrode 110, an organic layer 120, a second electrode 130, and a layer 140. The substrate 100 includes a first surface 102 and a second surface 104. The second surface 104 is on the opposite side of the first surface 102. The first electrode 110 is above the first surface 102 of the substrate 100. The second electrode 130 is above the first electrode 110. The organic layer 120 is between the first electrode 110 and the second electrode 130. The organic layer 120 includes a hole injection layer (HIL) 122, a hole transporting layer (HTL) 124, a light-emitting layer (EML) 126, and an electron transporting layer (ETL) 128.

The light-emitting device 10 includes the resonator 150. The resonator 150 includes a reflecting layer 152, a semi-transparent reflecting layer 154, and a first layer 156 (1) to a fifth layer 156 (5). The resonator 150 is configured of a first electrode 110, an organic layer 120, a second electrode 130, and a layer 140. Specifically, the second electrode 130 functions as the reflecting layer 152. The layer 140 functions as the semi-transparent reflecting layer 154. The first electrode 110 functions as the first layer 156 (1). The HIL 122, the HTL 124, the EML 126, and the ETL 128 function as a second layer 156 (2), a third layer 156 (3), a fourth layer 156 (4), and a fifth layer 156 (5), respectively.

The substrate 100 has light-transmitting properties, and specifically, for example, is a glass substrate or a resin substrate. The substrate 100 may or may not have flexibility. The thickness of the substrate 100 is, for example, equal to or greater than 10 μm and equal to or less than 1 mm.

The first electrode 110 has light-transmitting properties, and formed of, for example, a metal oxide, more specifically, for example, an indium tin oxide (ITO), an indium zinc oxide (IZO), an indium tungsten zinc oxide (IWZO), or a zinc oxide (ZnO).

The organic layer 120 includes an HIL 122, an HTL 124, an EML 126, and an ETL 128. However, the layer structure of the organic layer 120 is not limited to this example. As an example, the organic layer 120 may include an electron injection layer (EIL) between the second electrode 130 and the ETL 128. In this example, the EIL functions as a sixth layer 156 (6). As another example, the organic layer 120 need not include a HIL 122 or a HTL 124. Further, as still another example, the organic layer 120 may include a hole blocking layer (HBL), an electron blocking layer (EBL), a buffer layer, a spacer layer, a light extraction improvement layer, an adhesive layer, or a color filter layer. In addition, the organic layer 120 may have a multi-unit structure having a plurality of light-emitting layers, and in this example, for example, two or more sets of the HIL 122, the HTL 124, the EML 126, and the ETL 128 may be included.

The second electrode 130 functions as the reflecting layer 152. The second electrode 130 is formed of a material that reflects light, such as a metal, for example, Al, Ag, an Al alloy, or an Ag alloy. The thickness of the second electrode 130 is thick to a certain degree, for example, equal to or greater than 70 nm and equal to or less than 200 nm. Thus, the second electrode 130 functions as the reflecting layer 152.

The layer 140 functions as the semi-transparent reflecting layer 154. In an example, the layer 140 is a metal thin film, and specifically, for example, an Ag thin film, an Au thin film, an Ag alloy thin film, or an Au alloy thin film. In this example, the thickness of the layer 140 is thin to a certain degree, and specifically, for example, thinner than the thickness of the second electrode 130, and more specifically, for example, equal to or greater than 5 nm and equal to or less than 50 nm. In a case where the film thickness of the layer 140 is thin as such, a portion of light incident on the layer 140 can be transmitted through the layer 140. Thereby, the layer 140 functions as the semi-transparent reflecting layer 154. In another example, the layer 140 may be a dielectric multilayer film including a high refractive index dielectric layer and a low refractive index dielectric layer laminated alternately. In this example also, the layer 140 can function as the semi-transparent reflecting layer 154.

FIG. 3 is a drawing to explain the derivation of Formula (1). In the drawing, k=3, and the resonator 150 includes a first layer 156 (1), a second layer 156 (2), and a third layer 156 (3). Meanwhile, in the present drawing, the reflecting layer 152 (FIG. 1 and FIG. 2) and the semi-transparent reflecting layer 154 (FIG. 1 and FIG. 2) are removed for ease of explanation.

In the example shown in the drawing, a mutually strengthening interference is generated by light emitted at a refractive angle θ₀ from the first layer 156 (1) to the medium having a refractive index n₀ (specifically, air). Thereby, the light distribution of light has a maximum value in the angle θ₀ direction.

Specifically, an optical path difference Δl₃ defined by the following Formula (2) is an integral multiple of a wavelength λ of the above-mentioned light.

$\begin{matrix} {\left\lbrack {{Formula}\mspace{20mu} 2} \right\rbrack\mspace{619mu}} & \; \\ {{\Delta\; l_{3}} = {{\sum\limits_{i = 1}^{3}\frac{2n_{i}d_{i}}{\cos\mspace{11mu}\theta_{i}}} - {n_{0}\sin\mspace{11mu}\theta_{0}{\sum\limits_{i = 1}^{3}{2d_{i}\tan\mspace{11mu}\theta_{i}}}}}} & (2) \end{matrix}$ The first term on the right side of Formula (2) is the sum of an optical path length between A and B, an optical path length between B and C, an optical path length between C and D, an optical path length between D and E, an optical path length between E and F, and an optical path length between F and G. The second term on the right side of Formula (2) is an optical path length between A and H. The optical path length between A and H is derived using AG=2d₁ tan θ₁+2d₂ tan θ₂+2d₃ tan θ₃, ∠AGH=θ₀, and AH=AGsin θ₀.

The first term on the right side of Formula (1) is derived by generalizing the right side of Formula (2) by applying the number of layers k of the layer 156 to the right side of Formula (2) and using Snell's law n₀ sin θ₀=n_(i) sin θ_(i). In addition, a second term on the right side of Formula (2) is derived by taking the phase shift amount of the reflecting layer 152 and the phase shift amount of the semi-transparent reflecting layer 154 into consideration.

In a case where the value ΔM is an integer in Formula (1), the mutually strengthening interference is generated by light emitted at the refractive angle θ₀. Thereby, the light distribution of light has a maximum value in the angle θ₀ direction. However, the value ΔM need not strictly match a specific integer. The value ΔM may be deviated from an integer m (m≥1) by, for example, ±⅛, and preferably, for example, ± 1/16.

Meanwhile, in an example, phase shift amounts φ_(S) and (PR may be determined based on tan φ_(S)=2n₁k_(S)/(n₁ ²−n_(S) ²−k_(S) ²), and tan φ_(R)=2n_(k)k_(R)/(n_(k) ²−n_(R) ²−k_(R) ²), respectively (n_(S): a refractive index of the semi-transparent reflecting layer 154, k_(S): an extinction coefficient of the semi-transparent reflecting layer 154, n_(R): a refractive index of the reflecting layer 152, k_(R): an extinction coefficient of the reflecting layer 152). In another example, the phase shift amounts φ_(S) and φ_(R) may be determined based on a measurement result using spectral ellipsometry.

FIG. 4 is a flowchart explaining an example of a method of designing the light-emitting device 10 shown in FIG. 1 and FIG. 2. First, a reference optical path length is determined so that the light distribution has a maximum value in the reference direction R (θ₀=0) (S10). The reference optical path length is an optical path length between the reflecting layer 152 and the semi-transparent reflecting layer 154, and is d′₁n₁+d′₂n₂+ . . . +d′_(k)n_(k) (d′_(i): the thickness of the i-th layer 156 (i)).

Next, the thicknesses d₁−d_(k) of each of layers 156 are determined based on the reference optical path length so that the light distribution has a maximum value in the angle θ₀ direction (S20). Specifically, the thicknesses d₁−d_(k) of each of the layers 156 are determined to satisfy Formula (3) below.

$\begin{matrix} {\left\lbrack {{Formula}\mspace{20mu} 3} \right\rbrack\mspace{619mu}} & \; \\ {{\sum\limits_{i = 1}^{k}{d_{i}\sqrt{n_{i}^{2} - {n_{0}^{2}\sin^{2}\;\theta_{0}}}}} = {\sum\limits_{i = 1}^{k}{d_{i}^{\prime}n_{i}}}} & (3) \end{matrix}$

Formula (3) is derived as follows. First, the value ΔM in a case where the light distribution has a maximum value in the reference direction R (θ₀=0) is the following Formula (4) based on Formula (1).

$\begin{matrix} {\left\lbrack {{Formula}\mspace{20mu} 4} \right\rbrack\mspace{619mu}} & \; \\ {{\Delta\;{M^{\prime}(0)}} = {{\frac{2}{\lambda}{\sum\limits_{i = 1}^{k}{d_{i}^{\prime}n_{i}}}} + {\frac{1}{2\pi}\left( {\phi_{S} + \phi_{R}} \right)}}} & (4) \end{matrix}$

Next, the value ΔM in a case where the light distribution in the angle θ₀ direction has a maximum value is the following Formula (5) based on Formula (1).

$\begin{matrix} {\left\lbrack {{Formula}\mspace{20mu} 5} \right\rbrack\mspace{619mu}} & \; \\ {{\Delta\;{M\left( \theta_{0} \right)}} = {{\frac{2}{\lambda}{\sum\limits_{i = 1}^{k}{d_{i}\sqrt{n_{i}^{2} - {n_{0}^{2}\sin^{2}\theta_{0}}}}}} + {\frac{1}{2\pi}\left( {\phi_{S} + \phi_{R}} \right)}}} & (5) \end{matrix}$ Formula (3) is derived by ΔM (θ₀=0)=ΔM′(0) using Formula (4) and Formula (5).

Meanwhile, when deriving Formula (3), the phase shift amounts φ_(S) and φ_(R) at ΔM (θ₀) are assumed to be equal to the phase shift amounts φ_(S) and φ_(R) at ΔM′(0), respectively. Thereby, when deriving Formula (3), the phase shift amounts φ_(S) and φ_(R) are dropped out. In other words, when determining the thicknesses d₁−d_(k) of each of the layers 156 using Formula (3), the phase shift amounts φ_(S) and φ_(R) need not be calculated.

In S20, the thicknesses d₁−d_(k) are determined by adjusting the thicknesses d′₁−d′_(k) determined in S10. In an example, to satisfy Formula (3), the thickness of a layer of the organic layer 120 that is the closest to the semi-transparent reflecting layer 154 (in the examples shown in FIG. 1 and FIG. 2, the second layer 156 (2)), and the thickness of a layer of the organic layer 120 that is the closest to the reflecting layer 152 (in the examples shown in FIG. 1 and FIG. 2, the fifth layer 156 (5)) may be adjusted. However, the thickness of a layer 156 other than the layers 156 described in this example may be adjusted.

Further, in S20, the thicknesses d₁−d_(k) may be determined so that the ratio between the optical path length from the center of the EML 126 to the reflecting layer 152 and the optical path length from the center of the EML 126 to the semi-transparent reflecting layer 154 is the same when the thicknesses are d′₁-d′_(k) and when the thicknesses are d₁−d_(k). By determining the thicknesses in this way, the carrier balance in the organic layer 120 may be inhibited from being changed between an element when θ₀=0 and an element when having a peak at the angle θ₀. Meanwhile, the number of layers adjusted in thickness may be increased in a multi-unit structure in which the organic layer 120 has a plurality of light-emitting layers EML. For example, in an example of a structure having two light-emitting layers in an organic layer 120 which is the so-called tandem unit structure, the thickness of any of the layers interposed between a first light-emitting layer and a second light-emitting layer may be adjusted in addition to the two layers explained in the above-mentioned example. In a structure having three light-emitting layers in an organic layer 120 which is the so-called tridem unit structure, the film thickness is preferably adjusted in two layers between the light-emitting layers in addition to the aforementioned two layers. Thus, in the multi-unit structure, layers in a number which is the sum of the number of the light-emitting layers plus one are preferably adjusted.

FIG. 5 is a table showing an example of the light-emitting device 10 illustrated in FIG. 1 and FIG. 2. FIG. 6 is a table showing a refractive angle in each layer of the light-emitting device 10 illustrated in FIG. 5. FIG. 7 is a table explaining an example of a method of designing the light-emitting device 10 shown in FIG. 5 using a method shown in FIG. 4. In the example shown in FIG. 7, the light-emitting device 10 is designed so that the light distribution has a maximum value at a design angle of 0 degrees to 70 degrees.

In the example shown in FIG. 5, the light-emitting device 10 includes a substrate 100, a semi-transparent reflecting layer 154 (layer 140), a first layer 156 (1) (a first electrode 110), a second layer 156 (2) (HIL 122), a third layer 156 (3) (HTL 124), a fourth layer (4) (EML 126), a fifth layer 156 (5) (ETL 128), and a reflecting layer 152 (second electrode 130).

FIG. 6 shows a refractive angle θ_(S) at the substrate 100, a refractive angle θ₁ at the first layer 156 (1), a refractive angle θ₂ on the second layer 156 (2), a refractive angle θ₃ on the third layer 156 (3), a refractive angle θ₄ on the fourth layer 156 (4), and a refractive angle θ₅ at the fifth layer 156 (5) in a case where light of a wavelength λ 630 nm is emitted at each refractive angle θ₀ at 0.0 to 70.0 degrees from the second surface 104 of the substrate 100. The refractive angles θ_(S) and θ₁-θ₅ may be calculated from n₀ sin θ₀=n_(i) sin θ_(i) based on Snell's law.

As shown in FIG. 7, the thickness d₂ of the second layer 156 (2) and the thickness d₅ of the fifth layer 156 (5) may be determined. Specifically, first, the reference optical path length is determined using an optical simulation so that the light distribution has a maximum value in the reference direction (θ₀=0) (S10 in FIG. 4). In other words, the thicknesses d′₁-d′₅ of each of layers 156 are determined so that the light distribution has a maximum value in the reference direction (θ₀=0). In the example shown in FIG. 7, the reference optical path length is 530 nm. Next, the thicknesses of each of layers 156 d₁−d₅ are determined to satisfy Formula (3) (S20 in FIG. 4).

In detail, after calculating the reference optical path lengths (that is, the thicknesses d′₁-d′₅), an optical path length ΔL satisfying the following Formula (6) is calculated.

$\begin{matrix} {\left\lbrack {{Formula}\mspace{20mu} 6} \right\rbrack\mspace{619mu}} & \; \\ {{{\sum\limits_{i = 1}^{k}{d_{i}^{\prime}\sqrt{n_{i}^{2} - {n_{0}^{2}\sin^{2}\;\theta_{0}}}}} + {\Delta\; L}} = {\sum\limits_{i = 1}^{k}{d_{i}^{\prime}n_{i}}}} & (6) \end{matrix}$

Formula (6) is derived by substituting d_(i)=d′_(i)+Δd_(i) in the left side of Formula (3). Thereby, the optical path length ΔL is as per Formula (7) below.

$\begin{matrix} {\left\lbrack {{Formula}\mspace{20mu} 7} \right\rbrack\mspace{619mu}} & \; \\ {{\Delta\; L} = {\sum\limits_{i = 1}^{k}{\Delta\; d_{i}\sqrt{n_{i}^{2} - {n_{0}^{2}\sin^{2}\;\theta_{0}}}}}} & (7) \end{matrix}$

By using Formula (6) and Formula (7), the thickness ΔD=Δd₁+Δd₂+ . . . +Δd_(k) to be added to the thicknesses d′₁-d′_(k) can be calculated so as to obtain the design angle of θ₀. In the example shown in FIG. 7, the thickness Δd₂ alone is added to the thickness d′₂ of the lowermost layer (the second layer 156 (2)) of the organic layer 120, the thickness Δd_(S) alone is added to the thickness d′_(S) of the uppermost layer (the fifth layer 156 (5)) of the organic layer 120, and Δd₁=Δd₃=Δd₄=0 is true regarding the other layers 156. As such, the thicknesses d₁−d₅ of each of the layers 156 are determined.

Meanwhile, in the example shown in FIG. 7, only the second layer 156 (2) (having a function as the HIL) and the fifth layer 156 (5) (having a function as the ETL) which are organic layers are added to ΔD as adjustment layers. This allows to facilitate adjustment of the film thickness compared to adjustment of the first layer 156 (1) (having a function as the first electrode 110) and to more easily prevent change in the carrier balance generated in a case where the film thickness is adjusted, compared to adjustment of the fourth layer 156 (4) (having a function as the EML). Further, here, the percentages of the film thickness ΔD added to the second layer 156 (2) and to the fifth layer 156 (5) are set as follows: for the second layer 156 (2), the percentage of thickness to be added is the percentage of the optical distance from a light-emitting position to the semi-transparent reflection film when an optical distance from a semi-transparent reflection film to a reflection electrode is set to 1; and for the fifth layer 156 (5), the percentage of thickness to be added is the percentage of the optical distance from the light-emitting position to the reflection electrode when an optical distance from a semi-transparent reflection film to a reflection electrode is set to 1. Thus, in the example shown in FIG. 7, the thicknesses d₁-d₅ are determined so that the ratio between the optical path length from the center of the fourth layer 156 (4) to the reflecting layer 152 and the optical path length from the center of the EML 126 to the semi-transparent reflecting layer 154 becomes 0.259:0.741.

FIG. 8 is a graph showing the light distribution of the light-emitting device 10 designed under the conditions shown in FIG. 7 using rectangular coordinates. In the graph, the luminous intensity of the vertical axis is standardized by the luminous intensity of the light distribution of the light-emitting device 10 in the reference direction R according to a comparative example. The light-emitting device 10 according to the comparative example is the same as the light-emitting device 10 according to the embodiment, except that the semi-transparent reflecting layer 154 is not included, that is, the resonator 150 is not configured.

As shown in the drawing, the light distributions of the light-emitting device 10 at the design angles of 0 degrees, 10 degrees, 20 degrees, 30 degrees, 40 degrees, 50 degrees, 60 degrees, and 70 degrees have maximum values at 0 degrees, 10 degrees, 20 degrees, 30 degrees, 35 degrees, 45 degrees, 55 degrees, and 60 degrees, respectively. Thus, in some design angles, an angle in the direction at which the light distribution has a maximum value corresponds with a design angle, and in other design angles, the angle in the direction at which the light distribution has a maximum value substantially corresponds with a design angle.

It may be said that the light-emitting device 10 is preferably designed so that the light distribution has a maximum value in the direction inclined at, for example, an angle equal to or greater than 5 degrees, preferably, for example, at an angle equal to or greater than 10 degrees from the reference direction R in view of increasing the sharpness of peaks in the light distribution. According to the results shown in the drawing, it may be said a difference between the shape of the light distribution having a maximum value in the reference direction R and the shape of the light distribution having a maximum value in the direction inclined from the reference direction R becomes smaller as the angle at which the light distribution has a maximum value becomes smaller. In contrast, in a case where the light-emitting device 10 is designed so that the light distribution has a maximum value in the direction having an inclination which is, for example, equal to or greater than 5 degrees, and equal to or less than 10 degrees from the reference direction R, the sharpness of the peak of the light distribution is high.

From the viewpoint of positively matching the angle at which the light distribution has a maximum value with the design angle, the light-emitting device 10 is preferably designed so that the light distribution has a maximum value in the direction having an inclination which is equal to or less than 60 degrees, preferably, less than 45 degrees from the reference direction. According to the results shown by the drawing, it may be said that the angle at which the light distribution has a maximum value has a tendency to be smaller than the design angle as the design angle becomes greater. In contrast, in a case where the light-emitting device 10 is designed so that the light distribution has a maximum value in the direction having an inclination which is equal to or less than 60 degrees, preferably, less than 45 degrees from the reference direction R, an angle at which the light distribution has a maximum value positively matches the design angle.

FIG. 9(a) and FIG. 9(b) are graphs showing angular distributions of chromaticity of the light-emitting device 10 designed under the conditions shown in FIG. 7. The chromaticity (x, y) of FIG. 9(a) and FIG. 9(b) is the chromaticity of the CIE 1931 color space.

In the example shown in the drawing, the light-emitting device 10 is designed so that the chromaticity (x, y) is (0.700, 0.300) at an angle which is equal to the design angle. Specifically, first, the light-emitting device 10 is designed so that the chromaticity (x, y) thereof at the design angle of 0 degrees is (0.700, 0.300). Next, the light-emitting device 10 at the design angle of 10 degrees-70 degrees is designed using the method shown in FIG. 4. As shown in the drawing of FIG. 9(a), angular distributions at the design angles of 10 degrees-70 degrees for a value x are similar to the angular distributions which are obtained by moving the angular distributions at the design angle of 0 degrees only by +10 degrees to +70 degrees, respectively. As shown in the drawing of FIG. 9(b), the angular distributions at the design angles of 10 degrees-70 degrees regarding a value y are similar to the angular distributions which are obtained by moving the angular distribution at the design angle of 0 degrees only by +10 degrees to +70 degrees, respectively. Thereby, the chromaticity (x, y) of the light-emitting device 10 at the design angles of 0 degrees-70 degrees is approximately (0.700, 0.300), respectively, at 0 degrees-70 degrees.

FIG. 10 is a graph showing a spectral distribution of each of the light-emitting device 10 according to the embodiment and the light-emitting device 10 according to the comparative example. In the example shown in the chart, the light-emitting device 10 according to the embodiment is designed so that the relationship of Formula (1) holds when θ₀=30 degrees and λ=630 nm. In contrast, the light-emitting device 10 according to the comparative example is the same as the light-emitting device 10 according to the embodiment, except that the semi-transparent reflecting layer 154 is not included, that is, the resonator 150 is not configured and the width of the organic layer 120 is different from that of the embodiment.

In the example shown in the diagram, each spectral distribution is a spectral distribution when observed from a direction inclined by 30 degrees (that is, an angle which is equal to the angle θ₀) from the reference direction. As shown in the graph, the wavelength at which the spectral distribution of the light-emitting device 10 according to the embodiment is a maximum value is substantially the same as the wavelength at which the spectral distribution of the light-emitting device 10 according to the comparative example is a maximum value, and is approximately 630 nm. Further, the maximum value of the spectral distribution of the light-emitting device 10 according to the embodiment is greater than the maximum value of the spectral distribution of the light-emitting device 10 according to the comparative example. As explained later, in a case where the light-emitting device 10 includes a light-transmitting unit, the area of a light-emitting region with respect to the area of the light-emitting device 10 is limited. There is a problem in achieving a light emission intensity required for the light-emitting device 10. By adopting the configuration of the light-emitting device 10 according to the present example, the intensity of the light emission can be strengthened even within the limitation of the area of the light-emitting region.

FIG. 11(a) is a graph (a distribution curve) showing a light distribution of each of the light-emitting device 10 according to the embodiment and the light-emitting device 10 according to the comparative example using polar coordinates. FIG. 11(b) is a graph of each light distribution shown in FIG. 11(a) using rectangular coordinates. In the example shown in the drawing, the light-emitting device 10 which is the same as the light-emitting device 10 used in the example shown in FIG. 10 is used.

As shown in FIG. 11(a), all of the light distributions of the light-emitting device 10 according to the embodiment and the light-emitting device 10 according to the comparative example are symmetric with respect to the reference direction R. In addition, as shown in FIG. 11(b), the light distribution of the light-emitting device 10 according to the embodiment has a maximum value in the direction inclined by ±25 degrees (that is, approximately ±30 degrees) from the reference direction R. In contrast, the light distribution of the light-emitting device 10 according to the comparative example has a maximum value in the reference direction R, and the luminous intensity of the light distribution monotonically decreases as the inclination from the reference direction R becomes greater. As shown in FIG. 11(a) and FIG. 11(b), the luminous intensity of the light distribution is asymmetric with the maximum value of the light-emitting device 10 according to the embodiment as the center. In other words, the luminous intensity of the light distribution comparatively gradually rises up to the maximum value, and after exceeding the maximum value, rapidly falls. By adopting such a configuration, the contrast of the light-emitting device 10 can be enhanced.

FIG. 12(a) and FIG. 12(b) are graphs of the angular distribution of chromaticity of each of the light-emitting device 10 according to the embodiment and the light-emitting device 10 according to the comparative example. The chromaticity (x, y) of FIG. 12(a) and FIG. 12(b) is the chromaticity of the CIE 1931 color space. In the examples shown in the graphs, the light-emitting device 10 which is the same as the light-emitting device 10 used in the example shown in FIG. 10 is used.

As shown in FIG. 12(a) and FIG. 12(b), the chromaticity (x, y) of the light-emitting device 10 according to the comparative example is substantially constant regardless of the angle from the reference direction (a direction of 0 degrees in the graph). In contrast, the chromaticity (x, y) of the light-emitting device 10 according to the embodiment depends on the angle from the reference direction (a direction of 0 degrees in the graph) and varies more greatly than the chromaticity (x, y) of the light-emitting device 10 according to the comparative example. Therefore, as explained using FIG. 9, in the case of the light-emitting device 10 according to the embodiment, the light-emitting device 10 needs to be designed so as to obtain a desired chromaticity. In the example shown in the graphs, the light-emitting device 10 is designed so as to obtain the chromaticity (0.700, 0.300) at the angle of 30 degrees.

FIG. 13(a) is a graph (a distribution curve) showing a light distribution of the light-emitting device 10 according to a modification example using polar coordinates. FIG. 13(b) is a graph showing the light distribution described in FIG. 13(a) using rectangular coordinates. In the example shown in the graphs, designs are made for a light-emitting device 10 at a design angle of 0 degrees and a light-emitting device 10 at a design angle of 20 degrees.

According to the results shown by the graph, in view of increasing the range in which the light distribution has a high luminous intensity, the light-emitting device 10 is preferably designed so that the light distribution thereof has a maximum value in the direction inclined at an angle equal to or less than 20 degrees, and more preferably, equal to or less than 15 degrees from the reference direction R. As shown in the graph, the light distribution of the light-emitting device 10 at the design angle of 20 degrees in a wide range, specifically, at approximately 0 degrees to 25 degrees, has substantially the same luminous intensity as the luminous intensity of the light distribution of the light-emitting device 10 of the design angle of 0 degrees at 0 degrees. Thus, in a case where the design angle is small, the range is increased in which the light distribution has a high luminous intensity.

Meanwhile, according to the results shown in FIG. 8, in view of increasing the range in which the light distribution has a high luminous intensity, the light-emitting device 10 is preferably designed so that the light distribution has a maximum value in the direction inclined at an angle equal to or greater than 10 degrees from the reference direction R. From the results shown in FIG. 8, it may be said that the light distribution of the light-emitting device 10 at a small design angle (for example, around 5 degrees) is substantially the same as that of the light-emitting device 10 at the design angle of 0 degrees. In contrast, in a case where the light-emitting device 10 is designed so that the light distribution thereof has a maximum value in the direction inclined at an angle equal to or greater than 10 degrees from the reference direction R, the light distribution is different from that of the light-emitting device 10 at the design angle of 0 degrees.

FIG. 14 is a drawing showing a first modification example of FIG. 1. As shown in the drawing, the first electrode 110 may be located between the first surface 102 of the substrate 100 and the layer 140 (the semi-transparent reflecting layer 154). In other words, in the example shown in the drawing, the first electrode 110 does not configure a resonator 150. In the example shown in the drawing, only the organic layer 120 (HIL 122, HTL 124, EML 126, and ETL 128) is between the reflecting layer 152 and the semi-transparent reflecting layer 154. The HIL 122, the HTL 124, the EML 126, and the ETL 128 function as a first layer 156 (1), a second layer 156 (2), a third layer 156 (3), and a fourth layer 156 (4), respectively.

FIG. 15 is a drawing showing a second modification example of FIG. 1. As shown in the drawing, the first electrode 110 (FIG. 1) need not be included. In the example shown in the drawing, the layer 140 functions as an electrode. Specifically, the layer 140 is a conductive film, for example, a metal thin film. In addition, the thickness of the layer 140 is thin to a certain degree, and is, specifically, thin enough to allow a portion of light incident on the layer 140 to be transmitted therethrough. Thereby, the layer 140 functions as an electrode, and also as a semi-transparent reflecting layer 154.

FIG. 16 is a drawing showing a third modification example of FIG. 1. As shown in the drawing, the first electrode 110 may be located between two layers (a layer 142 and a layer 144). The layer 142 is between the first electrode 110 and the organic layer 120. The layer 144 is between the first surface 102 of the substrate 100 and the first electrode 110. The layer 142 functions as a semi-transparent reflecting layer 154. The layer 144 may function as an auxiliary electrode of the first electrode 110. In such a case, the layer 144 may be formed on a portion of the first electrode 110 and the substrate 100. Therefore, in the example shown in the drawing, the first electrode 110 does not configure a resonator 150.

FIG. 17(a) is a drawing explaining a first example of the reference direction R shown in FIG. 2. In the example shown in the drawing, the second surface 104 of the substrate 100 is a plane. In the example shown in the drawing, the reference direction R is a vertical direction or the normal direction of the second surface 104 of the substrate 100. Since the second surface 104 of the substrate 100 is a plane, the reference direction R is the same in all the regions in the second surface 104 of the substrate 100.

FIG. 17(b) is a drawing explaining a second example of the reference direction R shown in FIG. 2. In the example shown in the drawing, the second surface 104 of the substrate 100 is a curved surface, and specifically, is projected outward. In the example shown in the drawing, the reference direction R is the vertical direction of a tangent of the second surface 104 of the substrate 100 or the normal direction of a tangent plane of the second surface 104 of the substrate 100. Since the second surface 104 of the substrate 100 is a curved surface, the reference direction R is different depending on the region in the second surface 104 of the substrate 100. That is, in the example shown in the drawing, the reference direction R is not limited to a certain direction.

FIG. 17(c) is a drawing explaining a third example of the reference direction R shown in FIG. 2. In the example shown in the drawing, the second surface 104 of the substrate 100 is a curved surface, and specifically, is curved convexly outward. In the example shown in the drawing, the reference direction R is the vertical direction of the tangent of the second surface 104 of the substrate 100 or the normal direction of the tangent plane of the second surface 104 of the substrate 100. Since the second surface 104 of the substrate 100 is a curved surface, the reference direction R is different depending on the region in the second surface 104 of the substrate 100. That is, in the example shown in the drawing, the reference direction R is not limited to a certain direction.

As stated above, according to the embodiment, the light distribution of light from the light-emitting device 10 is higher in luminous intensity in a direction different from the reference direction R compared to that in the reference direction R. Thus, the light distribution of light from the light-emitting device 10 has a maximum value in the direction different from the central direction of this light distribution.

Example 1

FIG. 18 is a plan view of a light-emitting device 10 according to Example 1. FIG. 19 is a cross-sectional view taken along line A-A of FIG. 18. FIG. 20 is a cross-sectional view taken along line B-B of FIG. 18. Meanwhile, FIG. 1 corresponds to an enlarged drawing of a portion of the light-emitting device 10 according to the present example. In the example shown in FIG. 19, each layer of an organic layer 120 (HIL 122, HTL 124, EML 126, and ETL 128) is not shown in the diagram for ease of explanation.

The light-emitting device 10 includes a substrate 100, a first electrode 110, a first terminal 112, a first wiring 114, an organic layer 120, a second electrode 130, a second terminal 132, a second wiring 134, a layer 140, and an insulating layer 160. The substrate 100 has light-transmitting properties. The first electrode 110 functions as a layer 156. The organic layer 120 functions as a layer 156. The second electrode 130 functions as a reflecting layer 152. The layer 140 functions as a semi-transparent reflecting layer 154. The reflecting layer 152, the semi-transparent reflecting layer 154, and the layer 156 configure a resonator 150.

The first electrode 110, the organic layer 120, the second electrode 130, and the insulating layer 160 include a first end 110 a, a first end 120 a, a first end 130 a, and a first end 160 a, respectively, and further includes a second end 110 b, a second end 120 b, a second end 130 b, and a second end 160 b, respectively. The second end 110 b, the second end 120 b, the second end 130 b, and the second end 160 b are located on the opposite sides of the first end 110 a, the first end 120 a, the first end 130 a, and the first end 160 a, respectively.

As shown in FIG. 18, the light-emitting device 10 includes a light-emitting element 170 on a first surface 102 of the substrate 100. The light-emitting element 170 includes a plurality of light-emitting units 172 and a plurality of light-transmitting units 174. The plurality of light-emitting units 172 and the plurality of light-transmitting units 174 are alternately aligned. More specifically, in light-emitting units 172 adjacent to each other, the first end 110 a, the first end 120 a, the first end 130 a, and the first end 160 a of one light-emitting unit 172 are aligned to face the second end 110 b, the second end 120 b, the second end 130 b, and the second end 160 b of the other light-emitting unit 172, respectively, through the light-transmitting unit 174.

The light-emitting unit 172 is configured of the first electrode 110, the organic layer 120, and the second electrode 130 in an opening 162 of the insulating layer 160. In other words, in the light-emitting unit 172, the first electrode 110, the organic layer 120, and the second electrode 130 overlap each other. The light-transmitting unit 174 is a region between the first end 130 a of one second electrode 130 and the second end 130 b of the other second electrode 130 of the light-emitting units 172 which are adjacent to each other. Meanwhile, in the example shown in FIG. 18, the shape of the light-emitting unit 172 (the opening 162 of the insulating layer 160) is rectangular.

In the example shown in FIG. 18, the shape of the light-emitting element 170 is defined as a rectangle having a pair of long sides and a pair of short sides. Specifically, the pair of long sides of the light-emitting element 170 is overlapped with the pair of short sides of each of the plurality of light-emitting units 172. One short side of the light-emitting element 170 is overlapped with a long side on the outer side of a light-emitting unit 172 at one end out of the plurality of light-emitting units 172. The other short side of the light-emitting element 170 is overlapped with a long side on the outer side of a light-emitting unit 172 at the other end out of the plurality of light-emitting units 172.

The first terminal 112 and the second terminal 132 are located on the opposite side of each other with the light-emitting unit 172 therebetween. The first terminal 112 and the second terminal 132 extend along the long side of the light-emitting element 170. The first terminal 112 is connected to each of a plurality of first electrodes 110 through each of a plurality of first wirings 114. The second terminal 132 is connected to each of a plurality of second electrodes 130 through each of a plurality of second wirings 134. Thereby, it is possible to apply voltage from the outside to the first electrode 110 through the first terminal 112 and the first wiring 114. In addition, it is possible to apply voltage from the outside to the second electrode 130 through the second terminal 132 and the second wiring 134.

As shown in FIG. 19, the first electrode 110 is located over the first surface 102 of the substrate 100 with the layer 140 interposed therebetween. The insulating layer 160 is located over the first surface 102 of the substrate 100 so that a portion of the first electrode 110 is exposed from the opening 162 of the insulating layer 160. The insulating layer 160 is formed using an organic insulating material, specifically, for example, a polyimide. The organic layer 120 is located over the first electrode 110 and the insulating layer 160 so that a portion thereof is embedded in the opening 162. The second electrode 130 is located over the organic layer 120 so that a portion thereof is embedded in the opening 162. Thus, the first electrode 110, the organic layer 120, and the second electrode 130 overlap each other in the opening 162 of the insulating layer 160, and configure the light-emitting unit 172. In other words, the insulating layer 160 defines the light-emitting unit 172. In addition, the light-emitting element 170 may include a conductive unit which functions as an auxiliary electrode of the first electrode 110, and in such a case, the conductive unit is preferably formed between the first electrode 110 and the insulating layer 160 and covered by the insulating layer 160.

The first end 110 a and the second end 110 b of the first electrode 110 are located further on the inner side than the first end 160 a and the second end 160 b of the insulating layer 160, respectively. Therefore, the first end 110 a and the second end 110 b of the first electrode 110 are not exposed from the insulating layer 160. Thereby, the first electrode 110 and the second electrode 130 are inhibited from short-circuiting.

In the example shown in the drawing, the first end 120 a and the second end 120 b of the organic layer 120 are located further on the inner side than the first end 160 a and the second end 160 b of the insulating layer 160, respectively. In other words, the width of the organic layer 120 is small to a certain degree. Therefore, it is possible to make the width of a portion of the organic layer 120 which is outside of the light-emitting unit 172 narrow. That is, it is possible to make the width of a portion which does not function as a portion of the light-emitting unit 172 narrow.

In the example shown in the drawing, the first end 130 a and the second end 130 b of the second electrode 130 are located further on the inner side than the first end 160 a and the second end 160 b of the insulating layer 160, respectively, and further on the inner side than the first end 120 a and the second end 120 b of the organic layer 120, respectively. Thus, in the example shown in the drawing, the width of the outer portion of the light-emitting unit 172, that is, the light-transmitting unit 174, is broad.

In the example shown in FIG. 19, the first surface 102 of the substrate 100 includes a first region 102 a, a second region 102 b, and a third region 102 c. The first region 102 a is a region from the first end 130 a to the second end 130 b of the second electrode 130. The second region 102 b is a region from the first end 130 a of the second electrode 130 to the first end 160 a of the insulating layer 160 and a region from the second end 130 b of the second electrode 130 to the second end 160 b of the insulating layer 160. The third region 102 c is a region from the first end 160 a of the insulating layer 160 of one light-emitting unit 172 out of light-emitting units 172 adjacent to each other to the second end 160 b of the insulating layer 160 of the other light-emitting unit 172.

In the example shown in FIG. 19, in a direction from one light-emitting unit 172 toward the other light-emitting unit 172, a distance between the first end 130 a of the second electrode 130 (a first reflection electrode) and the first end 160 a of the insulating layer 160 (that is, a width d2 of the second region 102 b) is shorter than a distance between the first end 160 a of the insulating layer 160 of the one light-emitting unit 172 and the second end 160 b of the insulating layer 160 of the other light-emitting unit 172 (that is, a width d3 of the third region 102 c). In addition, in a direction from the other light-emitting unit 172 toward the one light-emitting unit 172, a distance between the second end 130 b of the second electrode 130 (a second reflection electrode) and the second end 160 b of the insulating layer 160 (that is, the width d2 of the second region 102 b) is shorter than a distance between the second end 160 b of the insulating layer 160 of the other light-emitting unit 172 and the first end 160 a of the insulating layer 160 of the one light-emitting unit 172 (that is, the width d3 of the third region 102 c). Thereby, the light transmittance of the light-emitting device 10 is high.

In detail, the light transmittance of the second region 102 b is lower than that of the third region 102 c. This is due to the insulating layer 160 being located in the second region 102 b while the insulating layer 160 is not located in the third region 102 c. As described above, the width d2 of the second region 102 b is narrower than the width d3 of the third region 102 c. Therefore, the light transmittance of the light-emitting device 10 is high.

Further, in the example shown in FIG. 19, the light-emitting device 10 is inhibited from functioning as a filter to shield light of a specific wavelength. In detail, there is a case where a light transmittance of the insulating layer 160 differs depending on the wavelength. Therefore, the insulating layer 160 may function as a filter to shield light of a specific wavelength. In the example shown in the drawing, as described above, the width d2 of the second region 102 b (a region overlapping the insulating layer 160) is narrow, and specifically, narrower than the width d3 of the third region 102 c. Therefore, the light-emitting device 10 is inhibited from functioning as a filter to shield light of a specific wavelength.

In the example shown in FIG. 19, the width d2 of the second region 102 b is, for example, equal to or greater than 0 times and equal to or less than 0.2 times of the width d1 of the first region 102 a (0≤d2/d1≤0.2). The width d3 of the third region 102 c is, for example, equal to or greater than 0.3 times and equal to or less than 2 times of the width d1 of the first region 102 a (0.3≤d3/d1≤2). The width d1 of the first region 102 a is, for example, equal to or greater than 50 μm and equal to or less than 500 μm. The width d2 of the second region 102 b is, for example, equal to or greater than 0 μm and equal to or less than 100 μm. The width d3 of the third region 102 c is equal to or greater than 15 μm and equal to or less than 1,000 μm.

In the present example, light from the light-emitting element 170, more specifically, from the light-emitting unit 172 is hardly emitted to a region on the first surface 102 side of the substrate 100, but is emitted to a region on the second surface 104 side of the substrate 100. This is due to light from the organic layer 120, specifically, the EML 126 shown in FIG. 1 and FIG. 2 being reflected by the second electrode 130 (the reflecting layer 152).

In addition, in the present example, light appears to be emitted across the whole surface of the light-emitting element 170 to the human eye. This is due to a plurality of light-emitting elements 170 being disposed at a narrow pitch.

In addition, in the present example, an object is viewed through the light-emitting device 10 by the human eye. In other words, the light-emitting device 10 functions as a semi-transparent OLED. This is due to the width of the second electrode 130 (the reflecting layer 152) being narrow to a certain degree and the light-transmitting unit 174 being located between the second electrodes 130 (the reflecting layers 152) adjacent to each other. Specifically, in a case where light is not emitted from the light-emitting element 170, an object on the first surface 102 side can be viewed by the human eye from the second surface 104 side through the light-emitting device. In addition, in either of a case where light is emitted from the light-emitting element 170 and a case where light is not emitted from the light-emitting element 170, an object on the second surface 104 side can be seen through the light-emitting device from the first surface 102 side by the human eye.

FIG. 21 is a drawing showing a first modification example of FIG. 19. In the example shown in the drawing, the first end 120 a and the second end 120 b of the organic layer 120 may be located further on the outer side than the first end 160 a and the second end 160 b of the insulating layer 160, respectively.

FIG. 22 is a drawing showing a second modification example of FIG. 19. In the example shown in the drawing, the organic layer 120 may extend across the two light-emitting units 172 adjacent to each other. More specifically, the organic layer 120 extends across the entire surface of the light-emitting element 170. In the example shown in the drawing, each of a plurality of organic layers 120 need not be formed on each of the plurality of first electrodes 110. Therefore, the alignment to form the organic layer 120 is facilitated. Further, by adopting such a configuration, a mask need not be washed when forming plural layers of the organic layers 120, thus reducing manufacturing steps. In addition, in the present invention, since the light-emitting direction of the light-emitting unit 172 changes depending on the film thickness of the organic layer 120, it is important to prevent nonuniformity in film formation. By eliminating a mask and performing vapor deposition over the light-emitting unit 172 and the light-transmitting unit 174 of the light-emitting element 170, nonuniform film formation of the organic layer 120 can be prevented, the nonuniform film formation caused by the mask, deviation of the mask, warping of the mask, and the like caused by the film forming environment of the organic layer 120, and alight emission with a high light emission intensity at a desired angle may be obtained with higher accuracy. Further, also in a case where a portion or an entirety of the organic layer 120 is deposited by a coating process, the organic layer 120 may be easily formed when the organic layer 120 is shaped to extend across the entire surface of the light-emitting element 170.

Example 2

FIG. 23 is a drawing showing a light-emitting system 20 according to Example 2. FIG. 24 is a cross-sectional view taken along line A-A of FIG. 23. FIG. 25 is a cross-sectional view taken along line B-B of FIG. 23. The light-emitting system 20 includes a light-emitting device 10, a base material 200, and a frame body 250.

The light-emitting device 10 according to the present example is the same as the light-emitting device 10 according to Example 1. The light-emitting device 10 is mounted on the base material 200. Specifically, the base material 200 includes a first surface 202 and a second surface 204. The second surface 204 is on the opposite side of the first surface 202. The light-emitting device 10 is mounted on the first surface 202 of the base material 200 so that a second surface 104 of a substrate 100 faces the first surface 202 of the base material 200. Meanwhile, in FIG. 23 to FIG. 25, the first electrode 110, the organic layer 120, the second electrode 130, the layer 140, and the insulating layer 160 are not shown for ease of explanation.

The base material 200 has light-transmitting properties. Therefore, light from the light-emitting unit 172 can be transmitted through the base material 200, and specifically, the light enters the first surface 202 of the base material 200 to the base material 200 and is emitted to the outside of the base material 200 through the second surface 204 of the base material 200.

The base material 200 is held by the frame body 250. In one example, the base material 200 functions as a window or a portion thereof. More specifically, in one example, the base material 200 functions as a window of a mobile object (for example, an automobile, a train, a ship, or an airplane), more specifically, a rear window of an automobile. In another example, the base material 200 functions as a window of a case for storing an object such as a commercial product (for example, a showcase) or a window of a house or a shop or a portion of the window. In a case where the base material 200 functions as a window, the base material 200 is required to be sturdy to a certain degree. Therefore, the thickness of the base material 200 is considerably thicker than that of the substrate 100, for example, equal to or greater than 2 mm and equal to or less than 50 mm.

The base material 200 includes a semi-transparent light-emitting region 240. The semi-transparent light-emitting region 240 includes a plurality of light-emitting regions 242 and a plurality of light-transmitting regions 244. The semi-transparent light-emitting region 240 is overlapped with a light-emitting element 170 of the light-emitting device 10. The light-emitting region 242 is overlapped with the light-transmitting unit 174 of the light-emitting device 10. In other words, the light-transmitting region 244 is not overlapped with the light-emitting unit 172 of the light-emitting device 10. Thus, the plurality of light-emitting regions 242 and the plurality of light-transmitting regions 244 are alternately aligned, as is the case with the plurality of the light-emitting units 172 and the plurality of the light-transmitting units 174.

As is the case with Example 1, light appears to be emitted across the whole surface of the semi-transparent light-emitting region 240 (the light-emitting element 170) to the human eye. In addition, an object is viewed through the semi-transparent light-emitting region 240 by the human eye. In other words, the semi-transparent light-emitting region 240 functions as a semi-transparent OLED. Specifically, in a case where light is not emitted from the semi-transparent light-emitting region 240 (the light-emitting element 170), an object on the first surface 202 side can be viewed through the light-emitting device by the human eye from the second surface 204 side. In addition, in either of a case where light is emitted from the semi-transparent light-emitting region 240 (the light-emitting element 170) and a case where light is not emitted from the semi-transparent light-emitting region 240 (the light-emitting element 170), an object on the second surface 204 side can be viewed from the first surface 202 side through the light-emitting device by the human eye. Further, the light-emitting system 20 may be mounted, in a case where the base material 200 is formed in the mobile object, without hindering the visibility of a passenger, particularly a driver, a steerer, and a pilot to the outside of the mobile object and the visibility of a shop clerk of a shop to the outside in a case where the base material 200 is a shop window.

In the example shown in FIG. 25, a standard direction S is a horizontal direction (a direction along X direction in the drawing). The base material 200 is supported by the frame body 250 so that the second surface 204 of the base material 200 is oriented obliquely upward from the standard direction S. Thereby, the reference direction R is oriented obliquely upward from the standard direction S. In addition, the thickness direction of the substrate 100, the thickness direction of the light-emitting unit 172, and the thickness direction of the base material 200 are oriented obliquely upward from the standard direction S. The reference direction R is a central direction of light distribution, and in the example shown in the drawing, for example, is a direction which is along any of the thickness direction of the substrate 100, the thickness direction of the light-emitting unit 172, and the thickness direction of the base material 200, or a normal direction of the second surface 204. Ina first direction D1, the light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) has a higher luminous intensity in the first direction D1 compared to that in the reference direction R, and specifically, the light distribution of light from the light-emitting region 242 has a maximum value in the first direction D1. Meanwhile, the standard direction S is not limited to the horizontal direction. For example, the standard direction S may be inclined from the horizontal direction.

In the example shown in the drawing, the first direction D1 is different from the reference direction R. Therefore, even when the base material 200 is inclined from a specific direction (for example, the standard direction S) as shown in the drawing, the light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) can have a high luminous intensity (for example, a maximum value) in a desired direction.

Further, in the example shown in the drawing, the first direction D1 is oriented in a direction different from the reference direction R, and is oriented in a direction which is substantially the same as the standard direction S. Specifically, an angle formed between the first direction D1 and the standard direction S is, for example, equal to or greater than 0 degrees and equal to or less than 5 degrees. Therefore, even when the base material 200 is inclined from the specific direction (for example, the standard direction S) as shown in the drawing, the light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) can have a high luminous intensity (for example, a maximum value) in the standard direction S (in the example shown in the drawing, the horizontal direction) or in the vicinity thereof. Meanwhile, such a light distribution is accomplished by allowing an inclination angle of the base material 200 from, for example, the vertical direction (Y direction in the drawing) to match or correspond with a design angle at which the light distribution has a maximum value (for example, refer to FIG. 5 to FIG. 7).

FIG. 26 is a graph explaining an example of the light distribution of the light-emitting system 20 shown in FIG. 25. The light distribution in the graph is a light distribution obtained by standardizing an angular distribution of the design angle of 30 degrees in FIG. 8. In the example shown in the graph, the standard direction S is the horizontal direction (a direction along X direction in FIG. 25). The reference direction R is oriented obliquely upward from the standard direction S (the horizontal direction). In the present example, the first direction D1 is oriented obliquely downward from the standard direction S (the horizontal direction).

The light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) has a higher luminous intensity in a direction different from the reference direction R, specifically, for example, in the standard direction S, compared to that in the reference direction R. Therefore, even when the base material 200 is inclined from the standard direction S, the light distribution in this case has a high luminous intensity in the standard direction S.

In addition, the light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) has a maximum value in the first direction D1. The first direction D1 is different from the standard direction S. Specifically, an angle formed between the first direction D1 and the reference direction R is greater than an angle formed between the standard direction S and the reference direction R. In other words, the first direction D1 is located farther from the reference direction R compared to the standard direction S, and further in other words, the standard direction S is between the reference direction R and the first direction D1.

In addition, the light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) is asymmetric with respect to the first direction D1. Specifically, in the example shown in FIG. 26, this light distribution has a first luminous intensity (approximately 0.20) in a direction which is 20 degrees from the first direction D1 toward the standard direction S, and has a second luminous intensity (approximately 0.85) in a direction which is 20 degrees from the first direction D1 toward a side opposite to the standard direction S. In the example shown in FIG. 26, the first luminous intensity (approximately 0.20) is smaller than the second luminous intensity (approximately 0.85).

Further, the light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) is substantially constant in the standard direction S and the vicinity thereof. Specifically, in the example shown in FIG. 26, this light distribution has a first standard luminous intensity (approximately 1.00) in the standard direction S, a second standard luminous intensity (approximately 0.90) in a direction which is 10 degrees from the standard direction S toward a first direction S1 side, and a third standard luminous intensity (approximately 0.90) in a direction which is 10 degrees from the standard direction S toward the reference direction R side. In the example shown in FIG. 26, all of the first standard luminous intensity (approximately 1.00), the second standard luminous intensity (approximately 0.90), and the third standard luminous intensity (approximately 0.90) are equal to or greater than 80% and equal to or less than 100% of the above-mentioned maximum value of the above-mentioned light distribution.

Meanwhile, also at a design angle other than 30 degrees, in a case where the first direction D1 is located farther compared to the standard direction S from the reference direction R, the light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) is substantially constant in the standard direction S and the vicinity thereof (for example, refer to FIG. 8).

In addition, the angle formed between the first direction D1 and the standard direction S is not limited to the example shown in the graph. The angle formed between the first direction D1 and the standard direction S may be set to, for example, equal to or greater than 2.5 degrees and equal to or less than 12.5 degrees, preferably, for example, equal to or greater than 5.0 degrees and equal to or less than 10 degrees.

FIG. 27(a) and FIG. 27(b) are graphs explaining examples of the angular distribution of chromaticity of the light-emitting system 20 shown in FIG. 25. The angular distributions in FIG. 27(a) and FIG. 27(b) are the angular distributions of the design angle of 30 degrees in FIG. 9(a) and FIG. 9(b). In the example shown in the graphs, the standard direction S is the horizontal direction (the direction along X direction in FIG. 25). The first side direction S1 is oriented obliquely upward from the standard direction S (the horizontal direction). The second side direction S2 is oriented obliquely downward from the standard direction S (the horizontal direction). Meanwhile, the standard direction S is not limited to the horizontal direction. For example, the standard direction S may be inclined from the horizontal direction.

Light from the light-emitting system 20 has standard chromaticity (x_(S), y_(S)) (approximately (0.710, 0.290)) in the standard direction S (θ_(S): 25 degrees). Further, light from the light-emitting system 20 has a first chromaticity (x_(S1), y_(S1)) (approximately (0.715, 0.285)), and a second chromaticity (x_(S2), y_(S2)) (approximately (0.695, 0.305)) in the first side direction S1 (e_(S1): 15 degrees) and the second side direction S2 (e_(S2): 35 degrees), respectively, the first side direction S1 and the second side direction S2 being symmetric with respect to the standard direction S. A difference between the first chromaticity (x_(S1), y_(S1)) and the standard chromaticity (x_(S), y_(S)) is smaller than a difference between the second chromaticity (x_(S2), y_(S2)) and the standard chromaticity (x_(S), y_(S)). In other words, in the example shown in the graphs, in exchange for an increased difference between the second chromaticity (x_(S2), y_(S2)) and the standard chromaticity (x_(S), y_(S)), the difference between the first chromaticity (x_(S1), y_(S1)) and the standard chromaticity (x_(S), y_(S)) is made small to a certain degree.

An angle formed between the first side direction S1 and the reference direction R is smaller than an angle formed between the second side direction S2 and the reference direction R. In other words, the first side direction S1 is located closer to the reference direction R compared to the second side direction S2.

The angular distribution of a value x is concaved downward in a range of approximately ±15 degrees from the design angle (30 degrees) and decreases monotonously. Therefore, when an angle θ_(S) of the standard direction S, an angle θ_(S1) of the first side direction S1, and an angle θ_(S2) of the second side direction S2 are located within this range, |x_(S1)−x_(S)|<|x_(S2)−x_(S)| is established. In addition, the angular distribution of a value y is convexed upward in a range of approximately ±15 degrees from the design angle (30 degrees) and increases monotonously. Therefore, when the angle θ_(S) of the standard direction S, the angle θ_(S1) of the first side direction S1, and the angle θ_(S2) of the second side direction S2 are located within this range, |y_(S1)−y_(S)|<|y_(S2)−y_(S)| is established. Thereby, the difference between the first chromaticity (x_(S1), y_(S1)) and the standard chromaticity (x_(S), y_(S)) is smaller than that between the second chromaticity (x_(S2), y_(S2)) and the standard chromaticity (x_(S), y_(S)) when the angle θ_(S) of the standard direction S, the angle θ_(S1) of the first side direction S1, and the angle θ_(S2) of the second side direction S2 are located within the range of approximately ±15 degrees from the design angle (30 degrees).

Meanwhile, at other design angles also, a difference between upper chromaticity (x_(U), y_(U)) and horizontal chromaticity (x_(H), y_(H)) is smaller than that of lower chromaticity (x_(D), y_(D)) and the horizontal chromaticity (x_(H), y_(H)) (for example, refer to FIG. 9(a) and FIG. 9(b)) when the angle θ_(S) of the standard direction 5, the angle θ_(S1) of the first side direction S1, and the angle θ_(S2) of the second side direction S2 are located within the range of approximately ±15 degrees from the design angle.

In addition, the angle formed between the first side direction S1 and the standard direction S (the angle formed between the second side direction S2 and the standard direction S) is not limited to the example shown in the graphs. Each of the angle formed between the first side direction S1 and the standard direction S and the angle formed between the second side direction S2 and the standard direction S is, for example, equal to or greater than 5 degrees and equal to or less than 15 degrees.

FIG. 28 is a drawing explaining a first example of a method of measuring the light distribution of light from the light-emitting region 242 (the light-emitting unit 172). In the example shown in the drawing, the second surface 204 of the base material 200 is inclined from a standard surface SS. The standard surface SS is, for example, a horizontal surface. The light-emitting region 242 includes a lower end A, an upper end B, and a center O between the lower end A and the upper end B on the second surface 204. The lower end A is located at a height hA from the standard surface SS. The upper end B is located at a height hB from the standard surface SS. The center O is located at a height ho from the standard surface SS. The light distribution of light from the light-emitting region 242 (the light-emitting unit 172) has a maximum value in a direction along the standard surface SS. In a case where the light distribution of light from the light-emitting region 242 (the light-emitting unit 172) has a maximum value in the direction along the standard surface SS, the luminous intensity measured by a photometer M is the maximum in a case where the photometer M is located at the height ho, compared to when the photometer M is located at any of the other heights (for example, hA or hB).

FIG. 29 is a drawing explaining a second example of the method of measuring the light distribution of light from the light-emitting region 242 (the light-emitting unit 172). As shown in the drawing, the light-emitting region 242 may be covered with a mask MSK except the center O and the vicinity thereof. Thereby, the light distribution of light only from the center O and the vicinity thereof can be measured.

FIG. 30 is a drawing showing a modification example of FIG. 25. As shown in the drawing, the first direction D1 and the standard direction S may correspond to each other. In the example shown in the drawing, the light distribution of light from the light-emitting region 242 (the light-emitting unit 172) can have a maximum value in the standard direction S (for example, the horizontal direction).

FIG. 31 is a drawing showing a first modification example of FIG. 24. As shown in the drawing, the light-emitting device 10 may be mounted on the second surface 204 of the base material 200. More specifically, in the example shown in the drawing, the light-emitting device 10 is mounted on the second surface 204 of the base material 200 so that the first surface 102 of the substrate 100 faces the second surface 204 of the base material 200 with the light-emitting element 170 interposed therebetween.

FIG. 32 is a drawing showing a second modification example of FIG. 24. As shown in the drawing, the light-emitting device 10 may be inside the base material 200. Specifically, in the example shown in the drawing, the base material 200 includes a first base material 210, a second base material 220, and an intermediate layer 230. The first base material 210 and the second base material 220 are, for example, glass plates. The intermediate layer 230 is, for example, a resin layer. Thereby, the base material 200 may function as laminated glass.

The first base material 210 includes a surface 212 and a surface 214. The surface 212 functions as the first surface 202 of the first base material 210. The surface 214 is on the opposite side of the surface 212. The second base material 220 includes a surface 222 and a surface 224. The surface 224 is on the opposite side of the surface 222 and functions as the second surface 204. The surface 214 of the first base material 210 and the surface 222 of the second base material 220 face each other with the light-emitting device 10 and the intermediate layer 230 interposed therebetween. More specifically, the light-emitting device 10 is mounted on the surface 222 of the second base material 220 so that the first surface 102 of the substrate 100 faces the surface 222 of the second laminated film 220. The first surface 102 of the substrate 100 and the light-emitting element 170 are covered with the intermediate layer 230.

FIG. 33 is a drawing showing a third modification example of FIG. 24. As shown in the drawing, the light-emitting element 170 may be formed directly on the first surface 202 of the base material 200. In other words, in the example shown in the drawing, the light-emitting device 10 does not include the substrate 100 (FIG. 24). Further in other words, in the example shown in the drawing, the base material 200 functions as the substrate 100.

Example 3

FIG. 34 is a cross-sectional view of a light-emitting system 20 according to Example 3, and corresponds to FIG. 25 of Example 2. The light-emitting system. 20 according to the present example is the same as the light-emitting system 20 according to Example 2 except the following point.

In the example shown in the drawing, a standard direction S is a horizontal direction (a direction along X direction in the drawing). A first direction D1 is oriented obliquely upward from the standard direction S (the horizontal direction). A first side direction S1 is oriented obliquely downward from the standard direction S (the horizontal direction). A second side direction S2 is oriented obliquely upward from the standard direction S (the horizontal direction). As shown in the drawing, a base material 200 may be supported so that a second surface 204 is oriented obliquely downward from the standard direction S. Thereby, a reference direction R is oriented obliquely downward from the standard direction S. Meanwhile, the standard direction S is not limited to the horizontal direction. For example, the standard direction S may be inclined from the horizontal direction.

A light distribution of light from a light-emitting region 242 (more specifically, a light-emitting unit 172) has a maximum value in the first direction D1. The first direction D1 is different from the standard direction S. Specifically, an angle formed between the first direction D1 and the reference direction R is greater than an angle formed between the standard direction S and the reference direction R. In other words, the first direction D1 is located farther from the reference direction R compared to the standard direction S. Thereby, due to the same reason as the reason explained using FIG. 25 and FIG. 26, in a light distribution of light from the light-emitting system 20, a luminous intensity in the standard direction S and a surrounding direction thereof is not remarkably changed.

Light from the light-emitting system 20 has a standard chromaticity in the standard direction S. In addition, the light from the light-emitting system 20 has a first chromaticity and a second chromaticity in the first side direction S1 and the second side direction S2, respectively, the first side direction S1 and the second side direction S2 being symmetric with respect to the standard direction S. An angle formed between the first side direction S1 and the reference direction R is smaller than an angle formed between the second side direction S2 and the reference direction R. In other words, the first side direction S1 is located closer to the reference direction R compared to the second side direction S2. Thereby, due to the same reason as the reason explained using FIG. 25 and FIG. 27, a difference between the first chromaticity and the standard chromaticity is smaller than a difference between the second chromaticity and the standard chromaticity.

FIG. 35 is a drawing showing a modification example of FIG. 34. As shown in the drawing, the first direction D1 and the standard direction S may correspond to each other. In the example shown in the drawing, the light distribution of light from the light-emitting region 242 (the light-emitting unit 172) can have a maximum value in the standard direction S (for example, the horizontal direction).

Example 4

Each of FIG. 36 and FIG. 37 is a cross-sectional view of a light-emitting system 20 according to Example 4, and corresponds to FIG. 24 and FIG. 25 of Example 2, respectively. The light-emitting system 20 according to the present example is the same as the light-emitting system 20 according to Example 2 except the following point.

In the example shown in the drawing, the light-emitting system 20 includes an optical member 180. The optical member 180 is a member to adjust a traveling direction of light, and specifically, for example, is a diffraction grating, a microprism, or a polarizing film. In the example shown in the drawings, a traveling direction of light from a light-emitting unit 172 is adjusted by the optical member 180 so that a light distribution from a second surface 204 has a higher luminous intensity in a direction different from a reference direction R, specifically, in the first direction D1 compared to that in the reference direction R. Therefore, even when a base material 200 is inclined from a specific direction (for example, the standard direction S) as shown in the drawing, a light distribution of light from a light-emitting region 242 can have a high luminous intensity (for example, a maximum value) in a desired direction.

In the example shown in the drawing, a light-emitting device 10 need not be designed so that a value ΔM of the above-mentioned formula (1) satisfies equal to or greater than m−⅛ and equal to or less than m+⅛ in a case where θ≠0 degrees. In one example, the light-emitting device 10 need not include a semi-transparent reflecting layer 154 (for example, FIG. 19), in other words, need not include a microcavity structure. In another example, the light-emitting device 10 may be designed so that the value ΔM satisfies equal to or greater than m−⅛ and equal to or less than m+⅛ in a case where θ=0 degrees in the above-mentioned formula (1). In any example, by using the optical member 180, the light distribution of light from the second surface 204 has a maximum value in the direction different from the reference direction R, specifically, in the first direction D1.

In the example shown in the drawing, the optical member 180 is formed not to be overlapped with a light-transmitting unit 174 (a light-transmitting region 244). Thereby, a light transmittance of the light-emitting system 20 is inhibited from decreasing. Meanwhile, in the example shown in the drawing, the optical member 180 is located between the second surface 104 of the substrate 100 and the first surface 202 of the base material 200.

Example 5

FIG. 38 is a drawing showing a mobile object 22 according to Example 5. In the example shown in the drawing, the mobile object 22 includes a body 260 and a light-emitting system 20. The light-emitting system 20 is held by the body 260. In the example shown in the drawing, the mobile object 22 is an automobile, and the body 260 is a vehicle body. The mobile object 22 moves on a road surface RS. Meanwhile, the mobile object 22 may be a train, a ship, or an airplane. In a case where the mobile object 22 is a train, the body 260 is a vehicle body of a train. In a case where the mobile object 22 is a ship, the body 260 is a hull. In a case where the mobile object 22 is an airplane, the body 260 is a fuselage.

In the example shown in the drawing, the standard direction S is the horizontal direction (the direction along X direction in the drawing). In addition, the standard direction S also is a direction along the road surface RS, a traveling direction of the mobile object 22, and a direction to the rear side of the mobile object 22. In a first direction D1, a light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) has a higher luminous intensity in the first direction D1 compared to that in the reference direction R, and specifically, has a maximum value in the first direction D1. In the example shown in the drawing, the base material 200 is supported so that the second surface 204 is oriented obliquely upward from the standard direction S. Thereby, the reference direction R is oriented obliquely upward from the standard direction S. Meanwhile, the standard direction S is not limited to the horizontal direction. For example, the standard direction S may be inclined from the horizontal direction.

In the example shown in the drawing, the first direction D1 is different from the reference direction R. Therefore, even when the base material 200 is inclined from a specific direction (for example, the standard direction S) as shown in the drawing, the light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) can have a high luminous intensity (for example, a maximum value) in a desired direction.

Further, in the example shown in the drawing, the first direction D1 is oriented in a direction different from the reference direction R, and is oriented ins a direction which is substantially the same as the standard direction S. Specifically, an angle formed between the first direction D1 and the standard direction S is, for example, equal to or greater than 0 degrees and equal to or less than 5 degrees. Therefore, even when the base material 200 is inclined from a specific direction (for example, the standard direction S) as shown in the drawing, the light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) can have a high luminous intensity (for example, a maximum value) in the standard direction S (in the example shown in the drawing, the horizontal direction) and in the vicinity thereof.

The mobile object 22 includes the body 260. A portion of the body 260 functions as a frame body 250. In the example shown in the drawing, the base material 200 is supported by the frame body 250, and functions as a rear window.

In the example shown in the drawing, the light-emitting unit 172 (the light-emitting region 242) configures a portion of an “auxiliary brake lamp” (in other words, a high-mount stop-lamp (HMSL) or a break lamp) prescribed in Article 39, Paragraph 2 of the Safety Standards of Road Transport Vehicle in Japan. The light-emitting unit 172 (specifically, the center of the light-emitting unit 172) is located at a height hL which is, for example, equal to or greater than 1 m and equal to or less than 1.2 m from the road surface RS on which the mobile body travels.

The light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) has a higher luminous intensity in the standard direction S compared to that in the reference direction R. Therefore, even when the base material 200 is mounted on the mobile object 22 inclined from the standard direction S, this light distribution has a high luminous intensity in the standard direction S which is a direction of traffic following the mobile object 22. Therefore, the luminous intensity of a light emission from the light-emitting region 242 (the light-emitting unit 172) is increased. In addition, the light is efficiently irradiated in a direction of the traffic that follows, and information on braking of the mobile object 22 can be efficiently communicated or displayed.

Further, in FIG. 38, the first direction D1 is oriented obliquely downward from the standard direction S (the horizontal direction). A first side direction S1 is oriented obliquely upward from the standard direction S (the horizontal direction). A second side direction S2 is oriented obliquely downward from the standard direction S (the horizontal direction). Here, the light distribution of light from the light-emitting region 242 (more specifically, the light-emitting unit 172) has a maximum value in the first direction D1. The first direction D1 is different from the standard direction S. Specifically, an angle formed between the first direction D1 and the reference direction R is greater than an angle formed between the standard direction S and the reference direction R. In other words, the first direction D1 is located farther from the reference direction R compared to the standard direction S. Thereby, due to the same reason as the reason explained using FIG. 25 and FIG. 26, in a light distribution of light from the light-emitting system 20, a luminous intensity in the standard direction S and a surrounding direction thereof is not remarkably changed. By adopting such a configuration, the light-emitting system 20 can display information on braking of the mobile object 22 to the traffic that follows without the traffic that follows being affected by the height of the viewpoint.

Light from the light-emitting system 20 has standard chromaticity in the standard direction S. In addition, the light from the light-emitting system 20 has first chromaticity and second chromaticity in the first side direction S1 and the second side direction S2, respectively, the first side direction S1 and the second side direction S2 being symmetric with respect to the standard direction S. An angle formed between the first side direction S1 and the reference direction R is smaller than an angle formed between the second side direction S2 and the reference direction R. In other words, the first side direction S1 is located closer to the reference direction R compared to the second side direction S2. Thereby, due to the same reason as the reason explained using FIG. 25 and FIG. 27, a difference between the first chromaticity and the standard chromaticity is smaller than a difference between the second chromaticity and the standard chromaticity.

As described above, although the embodiment and examples of the present invention have been set forth with reference to the accompanying drawings, they are merely illustrative of the present invention, and various configurations other than those stated above can be adopted. 

The invention claimed is:
 1. A light-emitting system comprising: a light-emitting unit comprising a resonator and an organic layer interposed in the resonator, the light-emitting unit inclined from a standard direction, wherein a light distribution of light from the light-emitting unit has a higher luminous intensity in the standard direction compared to that in a reference direction along a width direction of any of the light-emitting unit, the resonator, or the organic layer, wherein the light from the light-emitting unit comprises standard chromaticity in the standard direction, the light from the light-emitting unit further comprising first chromaticity and second chromaticity in a first side direction and a second side direction, respectively, the first side direction and the second side direction being symmetric with respect to the standard direction, and wherein a difference between the first chromaticity and the reference chromaticity is smaller than a difference between the second chromaticity and the reference chromaticity.
 2. The light-emitting system according to claim 1, wherein the first side direction is oriented obliquely upward from a horizontal direction, and the second side direction is oriented obliquely downward from the horizontal direction.
 3. The light-emitting system according to claim 1, wherein the first side direction is oriented obliquely downward from a horizontal direction, and the second side direction is oriented obliquely upward from the horizontal direction.
 4. The light-emitting system according to claim 1, wherein each of an angle formed between the first side direction and the standard direction and an angle formed between the second side direction and the standard direction is equal to or greater than 5 degrees and equal to or less than 15 degrees.
 5. The light-emitting system according to claim 1, further comprising a reflecting layer and a semi-transparent reflecting layer, wherein the organic layer is between the reflecting layer and the semi-transparent reflecting layer, the organic layer comprising a light-emitting layer.
 6. The light-emitting system according to claim 5, further comprising k layers from a first layer to a k-th layer (k is an integer that is equal to or greater than 2) between the semi-transparent reflecting layer and the reflecting layer, wherein a value ΔM defined by Formula (1) below is equal to or greater than m−1/8 and equal to or less than m+1/8 (m is an integer that is equal to or greater than 1): $\begin{matrix} {\left\lbrack {{Formula}\mspace{20mu} 1} \right\rbrack\mspace{619mu}} & \; \\ {{\Delta\; M} = {{\frac{2}{\lambda}{\sum\limits_{i = 1}^{k}{d_{i}\sqrt{n_{i}^{2} - {n_{0}^{2}\sin^{2}\theta_{0}}}}}} + {\frac{1}{2\pi}\left( {\phi_{S} + \phi_{R}} \right)}}} & (1) \end{matrix}$ λ: peak wavelength of light from the light-emitting unit d_(i): thickness of i-th layer (1≤i≤k) n_(i): refractive index of i-th layer (1≤i≤k) n₀: refractive index of medium propagated by light from the light-emitting layer θ₀: angle of direction at which the light distribution has a maximum value φ_(s): phase shift amount of the semi-transparent reflecting layer φ_(R): phase shift amount of the reflecting layer.
 7. The light-emitting system according to claim 6, wherein the light distribution has a higher luminous intensity in a second direction on an opposite side of the first direction from the reference direction compared to a luminous intensity in the reference direction.
 8. The light-emitting system according to claim 1, further comprising a plurality of the light-emitting units and a plurality of light-transmitting units, wherein the plurality of light-emitting units comprise a first light-emitting unit and a second light-emitting unit that is adjacent to the first light-emitting unit, and wherein the plurality of light-transmitting units comprise a first light-transmitting unit between the first light-emitting unit and the second light-emitting unit.
 9. The light-emitting system according to claim 1, wherein the light-emitting unit is installed on a mobile object, and wherein the light-emitting unit is located at a height of equal to or greater than 1 m and equal to or less than 1 m 20 cm from a road surface on which the mobile object travels.
 10. The light-emitting system according to claim 1, wherein the standard direction is a horizontal direction. 